Bloch Oscillations Alan Wu April 14, 2009 Physics 138.

Slides:



Advertisements
Similar presentations
Electrical and Thermal Conductivity
Advertisements

The Quantum Mechanics of Simple Systems
The photon, the quantum of light
High Intensity Laser Electron Scattering David D. Meyerhofer IEEE Journal of Quantum Electronics, Vol. 33, No. 11, November 1997.
Graphene: why πα? Louis Kang & Jihoon Kim
Computational Solid State Physics 計算物性学特論 第2回 2.Interaction between atoms and the lattice properties of crystals.
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Quantum electrodynamics.
Optical Engineering for the 21st Century: Microscopic Simulation of Quantum Cascade Lasers M.F. Pereira Theory of Semiconductor Materials and Optics Materials.
1 Fermi surfaces and Electron dynamics  Band structure calculations give E(k)  E(k) determines the dynamics of the electrons  It is E(k) at the Fermi.
One assumes: (1) energy, E  (- ℏ /i)  /  t (2) momentum, P  ( ℏ /i)  (3) particle probability density,  (r,t)  = i  /  x + j  /  y + k  / 
Solid state Phys. Chapter 2 Thermal and electrical properties 1.
No friction. No air resistance. Perfect Spring Two normal modes. Coupled Pendulums Weak spring Time Dependent Two State Problem Copyright – Michael D.
§5.6 §5.6 Tight-binding Tight-binding is first proposed in 1929 by Bloch. The primary idea is to use a linear combination of atomic orbitals as a set of.
Lecture 15: Electromagnetic Radiation
Lecture 16: Electromanetic Radiation Reading: Zumdahl 12.1, 12.2 Outline –The nature of electromagnetic radiation. –Light as energy. –The workfunction.
Modern Physics 6a – Intro to Quantum Mechanics Physical Systems, Thursday 15 Feb. 2007, EJZ Plan for our last four weeks: week 6 (today), Ch.6.1-3: Schrödinger.
Guillermina Ramirez San Juan
Schrödinger We already know how to find the momentum eigenvalues of a system. How about the energy and the evolution of a system? Schrödinger Representation:
Heisenberg Uncertainty Principle Heisenberg (1926) thought about measuring simultaneously the position and momentum (velocity) of an electron. Realization.
Electromagnetic radiation l MAXWELL'S EQUATIONS: are four differential equations summarizing nature of electricity and magnetism: (formulated by James.
1 Lecture IX dr hab. Ewa popko Electron dynamics  Band structure calculations give E(k)  E(k) determines the dynamics of the electrons.
Chang-Kui Duan, Institute of Modern Physics, CUPT 1 Harmonic oscillator and coherent states Reading materials: 1.Chapter 7 of Shankar’s PQM.
Optical Lattices 1 Greiner Lab Winter School 2010 Florian Huber 02/01/2010.
Quantum Mechanics (14/2) CH. Jeong 1. Bloch theorem The wavefunction in a (one-dimensional) crystal can be written in the form subject to the condition.
Specific Heat of Solids Quantum Size Effect on the Specific Heat Electrical and Thermal Conductivities of Solids Thermoelectricity Classical Size Effect.
Ch 9 pages Lecture 22 – Harmonic oscillator.
1 Chapter 3 Electromagnetic Theory, Photons and Light September 5,8 Electromagnetic waves 3.1 Basic laws of electromagnetic theory Lights are electromagnetic.
CHM 108 SUROVIEC FALL 2015 Quantum Mechanical Model.
Ch ; Lecture 26 – Quantum description of absorption.
Electronic Band Structures electrons in solids: in a periodic potential due to the periodic arrays of atoms electronic band structure: electron states.
مدرس المادة الدكتور :…………………………
Wave-Particle Duality - the Principle of Complementarity The principle of complementarity states that both the wave and particle aspects of light are fundamental.
1 Prof. Ming-Jer Chen Department of Electronics Engineering National Chiao-Tung University 02/17/ /17/2014 IEE5501 Solid State Physics Lecture 1:
ELECTRON THEORY OF METALS 1.Introduction: The electron theory has been developed in three stages: Stage 1.:- The Classical Free Electron Theory : Drude.
Wave Physics PHYS 2023 Tim Freegarde.
The quantum kicked rotator First approach to “Quantum Chaos”: take a system that is classically chaotic and quantize it.
For review of Schrodinger equation: monroecc
5. Quantum Theory 5.0. Wave Mechanics
4. Phonons Crystal Vibrations
Electromagnetism Around 1800 classical physics knew: - 1/r 2 Force law of attraction between positive & negative charges. - v ×B Force law for a moving.
1 Aims of this lecture The diatomic chain –final comments Next level of complexity: –quantisation – PHONONS –dispersion curves in three dimensions Measuring.
1 2. Atoms and Electrons How to describe a new physical phenomenon? New natural phenomenon Previously existing theory Not explained Explained New theoryPredicts.
Wednesday, Apr. 6, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #17 Wednesday, Apr. 6, 2005 Dr. Jae Yu Symmetries Local gauge symmetry Gauge.
Energy Gaps Insulators & Superconductors When does an energy or band gap lead to insulating behavior? Band gap insulators, Peierls’ insulators When does.
Phonons Packets of sound found present in the lattice as it vibrates … but the lattice vibration cannot be heard. Unlike static lattice model , which.
Solid State Physics Lecture 15 HW 8 Due March 29 Kittel Chapter 7: 3,4,6 The free electron standing wave and the traveling wave are not eigenstates.
Generation and control of high- order harmonics by the Interaction of infrared lasers with a thin Graphite layer Ashish K Gupta & Nimrod Moiseyev Technion-Israel.
Compton Effect X-Ray Scattering Classical Theory (cont’d): c) The scattered radiation should have the same frequency as the incident radiation d) Because.
Semiclassical dynamics in the presence of loss and gain Eva-Maria Graefe Department of Mathematics, Imperial College London, UK Non-Hermitian Photonics.
Raman Effect The Scattering of electromagnetic radiation by matter with a change of frequency.
Review of solid state physics
Materials Considerations in Semiconductor Detectors
Time Dependent Two State Problem
Chapter 3 Energy Band Theory.
5. Wave-Particle Duality - the Principle of Complementarity
Concept test 15.1 Suppose at time
Modelling & Simulation of Semiconductor Devices
Review of Semiconductor Physics
Quantum Superposition and Optical Transitions
Band Theory The other approach to band theory solves the Schrodinger equation using a periodic potential to represent the Coulomb attraction of the positive.
Elements of Quantum Mechanics
Concept test 15.1 Suppose at time
Fourier transforms and
Quantum Mechanical Treatment of The Optical Properties
More Quantum Mechanics
Energy Band 7 In free electron model, electrons occupy positive energy levels from E=0 to higher values of energy. They are valence electron so called.
Chapter 5 - Phonons II: Quantum Mechanics of Lattice Vibrations
5. Wave-Particle Duality - the Principle of Complementarity
Group theory for the periodic lattice
Atilla Ozgur Cakmak, PhD
Presentation transcript:

Bloch Oscillations Alan Wu April 14, 2009 Physics 138

Outline Phenomenon Description Semi-Classical Derivation Wannier-Stark States Implications and Applications –Terahertz Oscillations –Bloch Oscillation Transistors

Bloch Oscillation Phenomenon Described by Bloch (1928) Imagine a particle in a periodic potential acted on by a constant force. Example: electrons in crystal lattice exposed to constant electric field Classically, we expect Ohmic behavior

Bloch Oscillation Phenomenon But quantum mechanics predicts that the particle will undergo an oscillation The periodicity causes the group velocity of the wavefunction to oscillate Ohmic behavior results from scattering

Bloch Oscillation Frequency Use invariance: shift 1 period d and shift energy ΔE Phase shift now Corresponding frequency is

Semi-Classical Derivation Schrodinger’s Equation can be transformed into the form: Known as the Acceleration Theorem, since it describes change in momentum Like classical relation between momentum and force

K-Space in a Lattice Potential periodicity in real space => periodicity in k-space Also known as a reciprocal lattice

The Brillouin Zone Brillouin Zone: a basic cell in the reciprocal lattice The dispersion relation gives an oscillating k within this zone

Kronig Penney Model The Kronig Penney model for a lattice can be used to find the potential in k-space. Source:

Dispersion in lattice

Wannier-Stark Resonance States At each well, a series of energies are available, much like that of a harmonic resonator. These states form what is known as a Wannier-Stark energy ladder.

Tight-binding model Consider just interactions between neighboring wells (known as Wannier representation) Also have energy difference from constant force

Experimental Confirmations Bloch oscillations have been observed in semiconductor lattices Shining a laser will excite the Wannier Stark states, which then oscillate. These oscillations can be measured

Terahertz Radiation Changing the electric field allows for a tunable radiation source. Can get frequencies in the terahertz

Bloch Oscillation Transistors Bloch oscillations can control Josephson Junctions Act much like bipolar transistors

Conclusion Bloch oscillations are just another strange quantum phenomenon They can be used for frequencies in the terahertz range Bloch oscillator transistors are an interesting way of amplifying signals